Chapter 18: Problem 18
(a) Show that the Alfvèn radius is given by Eq. (39). $$r_{A}=\left(\frac{8 \pi^{2} B_{s}^{4} R^{12}}{\mu_{0}^{2} G M \dot{M}^{2}}\right)^{1 / 7}$$ (b) Show that \(\dot{P} / P\) for the spin-up of an X-ray pulsar is given by Eq. (41). $$\frac{\dot{P}}{P}=-\frac{P \sqrt{\alpha}}{2 \pi I}\left(\frac{2 \sqrt{2} \pi B_{s}^{2} R^{6} G^{3} M^{3} \dot{M}^{6}}{\mu_{0}}\right)^{1 / 7}.$$
Short Answer
Step by step solution
Understand Alfvèn radius
Derive the Alfvèn radius equation
Simplify to match Eq. (39)
Understand \(\dot{P} / P\) for spin-up
Derive the expression for \(\dot{P} / P\)
Match Eq. (41)
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Magnetic Pressure
- Understanding magnetic pressure helps balance forces in space, especially near stars where strong magnetic fields exist.
- The Alfvèn radius is a point where magnetic pressure equals the dynamic pressure of inflowing material.
Dynamic Pressure
- This type of pressure is especially relevant when considering the kinetic energy of material infalling towards a star or a pulsar.
- In the context of accretion, dynamic pressure is vital to determine how material interacts with magnetic and gravitational influences.
- At the Alfvèn radius, dynamic pressure is balanced by magnetic pressure, setting the stage for complex interactions in stellar environments.
Mass Accretion Rate
- The density \(\rho\) of infalling material, calculated as \(\rho = \frac{\dot{M}}{4\pi r^{2}v}\).
- The velocity \(v\) of the material, since accretion affects how fast material travels.
Pulsar Spin-up
- The equation includes factors like the Alfvèn radius, magnetic field strength \(B_s\), and the mass accretion rate \(\dot{M}\).
- Pulsar spin-up reveals the intimate link between accretion processes and stellar rotation dynamics.